CN103392276A - Tunable pump light source for optical amplifier - Google Patents

Abstract

A tunable external cavity laser for use as a pump laser in an optical amplifier, such as a raman amplifier or an erbium doped fibre amplifier, comprises a semiconductor gain device (12) operable to provide optical amplification, a diffraction grating (18) for selecting an operating wavelength of the laser and a MEMS actuator for changing the selected wavelength. Multiple gain devices may be coupled together to increase the bandwidth or gain of the optical amplifier.

Description

The adjustable pump light source that is used for image intensifer

Technical field

The present invention relates to be used in the pump light source in image intensifer, more specifically but not exclusively relate to being used in and mix jade or pearl earring fiber amplifier or the Raman adjustable pump light source in amplifying.

Background technology

Optical transmission system need to amplify to compensate or overcome light loss, for example appears at loss, connector loss or parts loss in optical fiber.

Wherein a kind of amplification method relates to direct amplifying optical signals, namely the signal of telecommunication is not applied to amplifier.

Optical transmission system need to amplify to overcome light loss, for example fibre loss, connector loss or parts loss.There are several selections in amplification, comprise that mixing jade or pearl earring fiber amplifier (EDFA), semiconductor optical amplifier and Raman amplifies.The disclosure provides for Raman amplifies the pump laser source with remarkable benefit.Owing to only needing a kind of variation just can meet needs as the several different pump laser that uses in the Amplifier Design of today, so parts have been simplified manufacturing.For the raman amplifier system, the disclosure has improved the system integration and improved systematic function can be provided.For EDFA, the disclosure can be used for according to finally being used for Optimal performance.

At least one pump light source that the raman amplifier system need to have an operative wavelength of restriction realizes amplifying, and usually need to have a different wave length realize the gain of the relative broad range of gain wavelength more than a pump light source.

Knownly provide a plurality of pump light sources, wherein each light source " locked " is to predetermined wavelength Fiber Bragg Grating FBG (Fibre Bragg Grating).

The purpose of this invention is to provide the adjustable pump light source in the image intensifer that is used in optical pumping.

Summary of the invention

The disclosure attempts to overcome or alleviate at least the problem of prior art.

According to an aspect of the present invention, provide the tunable light source that is used in image intensifer.This tunable light source comprises gain equipment, wavelength selector and output coupler.Gain equipment can operate to provide light amplification, and comprises gain media and the first reflecting surface.Wavelength selector is configured to select the part from the light of gain equipment.Output coupler will be directed to the light transmission device to be used for being coupled to image intensifer from the part of the selected part of the light of gain equipment, and another part is directed to wavelength selector.Gain equipment, output coupler and wavelength selector form resonator.Output coupler can comprise beam splitter.

Tunable light source can comprise two or more optical resonators, and each optical resonator comprises the gain equipment of the part that forms corresponding resonator, wherein from the light of each resonator output, is coupled by combiner and is directed to the light transmission device.

Alternatively, tunable light source also comprises for the actuator of change from the wavelength of the selected part of the light of gain equipment.

Alternatively, actuator is around the axle rotation wavelength selector of the direction of propagation perpendicular to light.

Alternatively, actuator rotating light redirector, this light-redirecting device is preferably speculum, and described light-redirecting device will be directed to from the light of gain equipment on wavelength selector, and wherein the light-redirecting device is around the axle rotation of the direction of propagation perpendicular to light.

Alternatively, actuator structurally makes wavelength selector be out of shape to change selected wavelength.

Alternatively, malformation comprises stretching, compression and/or crooked wavelength selector.Preferably, tunable light source also comprises for prevent the isolator that feeds back when light source is used in image intensifer.Alternatively, output coupler is beam splitter.Alternatively, output coupler is reflection-type diffraction grating.Alternatively, the light-redirecting device is directed to the light transmission device with light.

According to a further aspect in the invention, provide the tunable light source that is used in image intensifer.This light source comprises two or more gain equipments that can operate to provide light amplification, and each gain equipment comprises gain media and the first reflecting surface.Two or more actuatable wavelength selectors are provided, and each actuatable wavelength selector is configured to select the part from the light of one of gain equipment.This light source also comprises at least one output coupler.Each output coupler, wavelength selector and gain equipment form resonator, and wherein output coupler will be directed to the light transmission device to be used for being coupled to image intensifer from the part of the light of each gain equipment.

According to an execution mode, the tunable light source that is used in image intensifer is provided, this tunable light source comprises: gain equipment, it can operate to provide light amplification, gain equipment to comprise gain media and first end and the second end, and first end forms an end of optical resonator; Lens, it is used for collimation from the radiation of the second end emission of gain equipment and radiation is directed to the beam splitter that serves as output coupler, is used for allowing the part effusion optical resonator of radiation and is used for remainder is retained in optical resonator; Reflection-type diffraction grating, the second end of optical resonator is selected and formed to its wavelength that is used for radiation; And actuator, it is coupled to reflection-type diffraction grating and can operates to change wavelength selects.

Alternatively, tunable light source comprises: the second gain equipment, and it can operate to provide light amplification, and this gain equipment comprises the second gain media and first end and the second end, and first end forms an end of the second optical resonator; The second lens, it is used for collimation from the radiation of the second end emission of the second gain equipment and radiation is directed to the second beam splitter that serves as the second output coupler, is used for allowing overflow the second optical resonator and be used for remainder is retained in the second optical resonator of the part of radiation; The second reflection-type diffraction grating, the second end of the second optical resonator is selected and formed to its wavelength that is used for radiation; And second actuator, its wavelength that is coupled to the second reflection-type diffraction grating and can operates to change the second optical resonator is selected.

Alternatively, tunable light source comprises for the combiner of combination from the radiation of the first and second optical resonators.

Alternatively, lens are directed to light in optical fiber.

Alternatively, tunable light source also comprises for prevent the isolator that feeds back when light source is used in image intensifer.Alternatively, the first and second beam splitters are offset to prevent with in the radiation coupling to the first of from the first or second optical resonator or another in the second optical resonator each other.

Alternatively, the reserve part of the first and second beam splitters reflected radiation on different directions, the reserve part of reflected radiation in the opposite direction alternatively.Alternatively, the first and second beam splitters are at the reserve part of identical direction reflected radiation.

Alternatively, described or each beam splitter reflexes to the reserve part of the radiation in each in the first and second optical resonators on the light-redirecting device, for example on speculum, described light-redirecting device be directed to radiation described or each reflection-type diffraction grating on, and wherein said or each actuator is coupled to described or each light-redirecting device.

Alternatively, the first beam splitter reflexes to the corresponding reserve part of radiation on the first light-redirecting device, for example on speculum, described the first light-redirecting device is directed to the radiation in the first optical resonator on the first reflection-type diffraction grating, and wherein the second beam splitter reflexes to the corresponding reserve part of radiation on the second light-redirecting device, for example on speculum, described the second light-redirecting device is directed to the radiation in the second optical resonator on the second reflection-type diffraction grating, and wherein the first and second actuators are coupled to respectively the first or second light heavily to device.

alternatively, the first beam splitter reflexes to the corresponding reserve part of radiation on the first light-redirecting device, for example on speculum, described the first light-redirecting device is directed to the radiation in the first optical resonator on reflection-type diffraction grating, and wherein the second beam splitter reflexes to the corresponding reserve part of radiation on the second light-redirecting device, for example on speculum, described the second light-redirecting device is directed to the radiation in the second optical resonator on reflection-type diffraction grating, make reflection-type diffraction grating form the part of the first and second optical resonators, and wherein the first and second actuators are coupled to respectively the first or second light and reset device.

According to another execution mode, the tunable light source that is used in image intensifer is provided, this tunable light source comprises: gain equipment, it can operate to provide light amplification, gain equipment to comprise gain media and first end and the second end, and first end forms an end of optical resonator; Lens, it is used for collimation from the radiation of the second end emission of gain equipment and radiation is directed to the reflection-type diffraction grating of selecting and serve as output coupler for the wavelength of radiation, allows the part effusion optical resonator of radiation and is used for remainder is retained in optical resonator; The light-redirecting device, speculum for example, it forms the second end of optical resonator; And actuator, it is coupled to the light-redirecting device and can operates to change wavelength selects.This tunable light source comprises: the second gain equipment, and it can operate to provide light amplification; The second gain equipment comprises the second gain media and first end and the second end, and first end forms an end of the second optical resonator; The second lens, it is used for collimation from the radiation of the second end emission of the second gain equipment and radiation is directed to the second reflection-type diffraction grating of selecting and serve as the second output coupler for the wavelength of radiation, allows part effusion second optical resonator of radiation and is used for remainder is retained in the second optical resonator; The second light-redirecting device, speculum for example, it forms the second end of the second optical resonator; And second actuator, its wavelength that is coupled to the second light-redirecting device and can operates to change the second optical resonator is selected, and wherein reflection-type diffraction grating forms the part of the first and second optical resonators.

Alternatively, tunable light source comprises for the combiner of combination from the radiation of the first and second optical resonators.

Alternatively, actuator comprises MEMS (micro electro mechanical system) (MEMS).

Alternatively, two or more optical resonators provide the light of different wave length, although in some embodiments, they can provide the light of Same Wavelength.

, according to an execution mode, provide the image intensifer that comprises tunable light source as described above.

According to another execution mode, the raman amplifier system that is used for amplifying optical signals is provided, it comprises and utilizes at least one tunable light source mentioned above as pump light source.

Alternatively, the raman amplifier system comprises two or more tunable light sources, and it is combined to increase the gain of amplifier system or the amplification of light signal.

Alternatively, the raman amplifier system comprises two or more tunable light sources, and it is combined to increase bandwidth, and light signal can be exaggerated on this bandwidth.

According to another execution mode, the Erbium-Doped Fiber Amplifier system that is used for amplifying optical signals is provided, it comprise utilize as front at tunable light source as herein described as pump light source with the bait atom for excitation fiber.

Description of drawings

Referring now to accompanying drawing, exemplary execution mode is described, wherein:

Figure 1A illustrates the schematic diagram of tunable light source;

Figure 1B illustrates the schematic diagram of the relation curve of the spectrum output intensity of the semiconductor gain equipment shown in Figure 1A and wavelength;

Fig. 1 C is illustrated in the schematic diagram of the relation curve of spectrum output intensity in the optical delivery fiber shown in Figure 1A of position, different angle of wavelength selector and wavelength;

Fig. 2 A illustrates the schematic diagram of another tunable light source;

Fig. 2 B illustrates the schematic diagram of the relation curve of the spectrum output intensity of each semiconductor gain equipment of Fig. 2 A and wavelength;

Fig. 2 C illustrates the schematic diagram of the relation curve of the interior spectrum input intensity of the optical delivery fiber shown in Fig. 2 A and wavelength;

Fig. 3 A illustrates the schematic diagram of another tunable light source;

Fig. 3 B illustrates the schematic diagram of the relation curve of the spectrum output intensity of each semiconductor gain equipment of Fig. 3 A and wavelength;

Fig. 3 C illustrates the schematic diagram of the relation curve of the interior spectrum input intensity of the optical delivery fiber shown in Fig. 3 A and wavelength;

Fig. 4 A illustrates the schematic diagram of another tunable light source;

Fig. 4 B illustrates the schematic diagram of the relation curve of the spectrum output intensity of each semiconductor gain equipment of Fig. 4 A and wavelength;

Fig. 4 C illustrates the schematic diagram of the relation curve of the interior spectrum input intensity of the optical delivery fiber shown in Fig. 4 A and wavelength;

Fig. 5 A illustrates the schematic diagram of another tunable light source;

Fig. 5 B illustrates the schematic diagram of the relation curve of the spectrum output intensity of each semiconductor gain equipment of Fig. 5 A and wavelength;

Fig. 5 C illustrates the schematic diagram of the relation curve of the interior spectrum input intensity of the optical delivery fiber shown in Fig. 5 A and wavelength;

Fig. 6 A illustrates the schematic diagram of another tunable light source;

Fig. 6 B illustrates the schematic diagram of the relation curve of the spectrum output intensity of each semiconductor gain equipment of Fig. 6 A and wavelength;

Fig. 6 C illustrates the schematic diagram of the relation curve of the interior spectrum input intensity of the optical delivery fiber shown in Fig. 6 A and wavelength;

Fig. 7 illustrates another tunable light source;

Fig. 8 is any the schematic diagram of image intensifer of tunable light source that comprises in Figure 1A to 7; And

Fig. 9 is the schematic diagram of gain spectra of image intensifer that comprises Fig. 8 of four tunable light sources with four different peak wavelengths.

Embodiment

Following discloses the detailed description of particular implementation of the present invention.To understand, disclosed execution mode is only the example of some aspect of the present disclosure mode that can be implemented, and does not represent the full list of all modes that the disclosure can be embodied.In fact, will understand, tunable light source as herein described may be embodied in various and optional form.Accompanying drawing is not necessarily pro rata, and some features can be exaggerated or minimize to illustrate the details of particular implementation.Known parts, material or method are not necessarily described in sufficient detail, in order to avoid making disclosure indigestibility.Any specific 26S Proteasome Structure and Function details disclosed herein should not be interpreted as restrictive, and as just the basis of claim with as for the instruction those of skill in the art, differently using representative basis of the present disclosure.

, with reference to Figure 1A, show the schematic diagram of the tunable light source 10 that comprises the optical cavity that is called as " optical cavity ".

Light source 10 comprises semiconductor gain equipment 12, and it is direct-gap seminconductor alternatively, such as but not limited to GaAs, aluminum gallium arsenide, gallium phosphide, indium gallium phosphide, gallium nitride, indium GaAs, indium arsenic gallium nitride, indium phosphide, phosphorus indium gallium, indium arsenic indium gallium.

The wavelength of desired operation is depended in the selection of material.In some embodiments, for example expect in the execution mode of pumping erbium-doped fiber, the wavelength of expectation will about 700nm to about 1500nm, more preferably at about 970nm to about 1000nm(980nm for example) or preferably at about 1460nm to 1500nm(1480nm for example) the near infrared spectrum district in.In optional execution mode, for example in pumping, must be used for the wavelength Raman amplifies, the wavelength of expectation will be in short wavelength infrared spectral regions 1-4 μ m, more preferably in 1400nm arrives the scope of 1500nm, more preferably, pumping wavelength is about 1455nm, in order to optimize the amplification in the C-band of about 1530-1565nm scope; This is because in the optical fiber based on silicon dioxide, and about 10 to the 15THZ for example frequency shift (FS)s of 13.2THZ (being equivalent to about 100nm wavelength shift) are obtained maximum gain.

It is contemplated that, gain equipment 12 will form from the diode with p-n junction, and this diode is utilizing emitted light in response to the stimulation of electric current.Gain equipment 12 is provided with for to it, supplying the electrical contact of induced current.Thefirst end face 11 of gain equipment 12 is arranged to the surface of high reflection, and preferably, this can realize by cutting open the material that forms gain equipment 12, to form smooth surface; In optional execution mode, reflectance coating can be coated.

Radiation is launched from thesecond end face 13 with divergent beams.These radiation divergent beams are bylens 14 collimations.Radiation through collimation then is directed onbeam splitter 16;Beam splitter 16 passes in the first of incident radiation beam, and bybeam splitter 16, is transmitted.The second portion of incident radiation beam is being reflected on the direction perpendicular to incident radiation beam substantially.Radiation uses thebeam splitter 16 that serves as output coupler " to be divided and pick out "; Power output efficiency and/or laser threshold level are determined by the transmission/reflectance atbeam splitter 16 places.

Reflecting part is directed on wavelength selector 18.In one embodiment, wavelength selector is reflection-type diffraction grating.Alternatively, diffraction grating " is glittered " to raise the efficiency; This also can improve the wavelength selectivity ofresonator.Wavelength selector 18 is arranged on moveable platform.Platform is rotatable, so that the adjusting radiation is incident on the angle on grating.It is contemplated that,wavelength selector 18 will be arranged on actuator for example on the MEMS micro-actuator; Wherein said micro-actuator can be coupled to control system.

Wavelength selector 18 along the path identical with incident beam (that is, with the incident radiation beam antiparallel) at least a portion diffraction of incident radiation beam is returned.18 diffraction of wavelength selector are incident on the narrow bandwidth of the radiation spectrum above it.

The wavelength of diffracted radiation laser beam can be regulated byrotation wavelength selector 18, so that the change radiation is incident on the angle onwavelength selector 18.

Wavelength selector 18 andbeam splitter 16 form resonator together with reflectingsurface 11, thereby form external cavity diode laser.

Optional light delay equipment can be between collimatinglens 14 andbeam splitter 16 or betweenwavelength selector 18 andbeam splitter 16.

The part of passing throughbeam splitter 16 transmission of radiation laser beam is focused on bylens 20 on the end of optical delivery fiber, and preferably,lens 20 are arranged to collect the radiation laser beam bybeam splitter 16 transmission, and radiation laser beam are focused in the acceptance cone of optical delivery fiber.Optical delivery fiber can be used for the part of passing throughbeam splitter 16 transmission of propagate radiation light beam.

Figure 1B illustrates the output spectrum of the gain equipment 12 that comprises gain media.Can see, the output spectrum of the resonator that forms when the reflectingsurface 11 with by gain equipment 12,wavelength selector 18 andbeam splitter 16 is relatively the time (as shown in Fig. 1 C), and gain equipment has wide bandwidth.

Fig. 1 C is for four different angle θ in the orientation ofwavelength selector 18₁, θ₂, θ₃, θ₄The spectrum of resonator is shown; The peak strength of spectrum appears at four different wavelength places.

Be incident on radiation onwavelength selector 18 bywavelength selector 18 diffraction.Radiation is dispersed, and that is to say, its wavelength is separated.The diffracted angle of radiation depends on its wavelength.This diffraction allows the wavelength of resonator to be selected or to regulate., for the optimum performance of system, can " adjust " wavelength of resonator.In using the execution mode of diffraction grating aswavelength selector 18, the diffracted angle of radiation also depends on grating space---the slit of grating or the interval between groove.Wavelength is selected therefore can realize by changing grating space.This can for example stretch by the malformation of light beam or Compressed grating is realized, identical effect can be by realizing with respect to the protruding ground of incident radiation or lowland curved raster.It is contemplated that, micro-actuator or MEMS can be used to realize the malformation ofwavelength selector 18.

By this way, only have the selected arrowband of wavelength to be directed and get back in gain equipment 12, make resonator produce the angle of according to wavelength selector, arranging with respect to folded light beam and the narrow bandwidth of the radiation of selecting.In optional execution mode,wavelength selector 18 can change with the distortion of grating and is directed the arrowband of getting back to the wavelength in gain equipment 12.

Fig. 2 A to 7 illustrates optional tunable light source.Second and subsequently shown in example in, similar numeral is used for representing similar parts in possible occasion, although the prefix of being added with " 100 " or " 200 " etc. are to indicate these features to belong to second or subsequently example.Optional execution mode and the first execution mode are shared a lot of public characteristics, therefore only have with the difference of the execution mode shown in Figure 1A and will be described in more detail.

Fig. 2 A illustrates the tunable light source that comprises a pair ofgain equipment 112A, 112B; Output radiation from eachgain equipment 112A, 128B is collimated by corresponding collimatinglens 114A, 114B.

Collimated light beam fromfirst lens 114A is directed to thefirst beam splitter 116A, and from the collimated light beam of thesecond lens 114B, is directed to thesecond beam splitter 116B.

Beam splitter 116A, 116B are arranged to reflect in the opposite direction corresponding incident beam.In optional execution mode, will recognize, light beam can be reflected on different directions.

, when the reflecting part of the light beam frombeam splitter 116B was directed to secondwave length selector 118B when upper, from the reflecting part of the light beam ofbeam splitter 116A, be directed on thefirst wavelength selector 118A.

Eachwavelength selector 118A, 118B are arranged on actuator to allow relative to each other independently rotation of eachwavelength selector 118A, 118B; This allows the diffraction wavelength of each resonator to be selected individually.

The reflecting surface of the reflecting surface 111A ofgain equipment 112A, the reflecting surface ofbeam splitter 116A andwavelength selector 118A forms the first resonator.

The reflecting surface of the reflecting surface 111B ofgain equipment 112B, the reflecting surface ofbeam splitter 116B andwavelength selector 118B forms the second resonator.

The output of each resonator is combined by beam combiner 124.Beam combiner 124 is optical polarization beam combiner preferably.In optional execution mode,beam combiner 124 can utilize space or wavelength combinations.

Then combination radiation frombeam combiner 124 passes isolator 126, and this prevents or reduce the feedback of radiation, and the image intensifer system of isolating pump light source and with pump light source, being coupled.

Condenser lens 120 redirects radiation, makes it can be trapped inoptical delivery fiber 122.

In unshowned optional execution mode, thefirst beam splitter 116A and thesecond beam splitter 116B are offset each other; They are arranged in from the different distance place of correspondingcollimating lens 114A, 114B.This prevents two cross-couplings between resonator, from any part of passing through thefirst beam splitter 116A transmission of the diffraction radiation of thefirst wavelength selector 118A of the first resonator, can not be coupled in the second resonator by thesecond beam splitter 116B; Skew also prevents from passing through thefirst beam splitter 116A cross-couplings to the first resonator from the radiation of second wave length selector diffraction.

In another execution mode, by filter being placed between thefirst beam splitter 116A and thesecond beam splitter 116B, can prevent cross-couplings.

Fig. 2 B illustrates the output spectrum of eachgain equipment 112A, 112B, and the output spectrum of each gain equipment can be not identical; The output spectrum of each gain equipment has the wide bandwidth up to about 10nm.

Fig. 2 C illustrates the spectrum that is input in optical delivery fiber 122.Two the different peak values at different wavelength places that provided by each resonator are provided spectrum, and each peak value has narrow bandwidth, and wherein the peak wavelength of each peak value can be conditioned.

It is contemplated that, from the spectrum of each resonator output, can be adjusted individually, make the peak wavelength from each resonator overlap at identical substantially wavelength place, thereby increase the intensity that is input to the radiation at the setted wavelength place in optical delivery fiber.

Fig. 3 A illustrates the optional configuration that is coupled for two resonators.In this embodiment, beam splitter 216A, 216B are arranged to make folded light beam to be redirected in the same direction, as the pair of parallel light beam.Compare from the distance of collimating lens 214B with beam splitter 216A, beam splitter 216B is arranged in the larger distance from collimating lens 214B.

Fig. 3 B illustrates the output spectrum of each gain equipment 212A, 212B, and the output spectrum of each gain equipment can be not identical; The output spectrum of each gain equipment has the wide bandwidth up to about 10nm.

Fig. 3 C illustrates the spectrum that is input in optical delivery fiber 222.Spectrum is included in two different peak values at different wavelength places, and each peak value has narrow bandwidth, and wherein the peak wavelength of each peak value can be conditioned.

Fig. 4 A illustrates tunable light source, wherein from the radiation laser beam ofbeam splitter 316 reflections, is directed on speculum 328.Speculum 328 is arranged on movable chassis, makesspeculum 328 to rotate around the axle of the direction of propagation perpendicular to radiation.Can again imagine, micro-actuator or MEMS can be used for realizing the rotation ofspeculum 328.

The advantage of this layout is better simply manufacturability and lower cost.The feature of the tunability that the wavelength selectivity that is provided bywavelength selector 18 as shown in Figure 1A, 2A and 3A will be provided and be provided by micro-actuator or MEMS in an assembly needs narrower manufacturing tolerance, and this has increased parts code requirement and cost.

It is relative simple that another advantage of using independent scanning MEMS speculum and body grating is that they manufacture.

Speculum 328 is directed towavelength selector 318 withradiation.Wavelength selector 318 is arranged on constant bearing.

Wavelength selector 318 is envisioned for reflection-type diffraction grating again, and it is arranged so that radiation and the incident radiation antiparallel of diffraction, namely along it from direction be reflected back toward.

Fig. 4 B illustrates the output spectrum of thegain equipment 312 that comprises gain media.Can see, the output spectrum of the resonator that forms when the reflectingsurface 311 with fromgain equipment 312,wavelength selector 318 andbeam splitter 316 andspeculum 328 is relatively the time (as shown in Figure 4 C), andgain equipment 312 has wide bandwidth.

Fig. 4 C illustrates the spectrum of resonator for four different angle θ 1, θ 2, θ 3, the θ 4 in the orientation ofspeculum 328; The peak strength of spectrum appears at four different wavelength places.

Fig. 5 A illustrates tunable light source, and whereinsingle wavelength selector 418 forms the part of each resonator in a pair of resonator.

Thefirst gain equipment 412A produces the radiation that is collimated and be directed to thefirst beam splitter 416A bylens 414A, make a part that is incident on the collimated light beam on thefirst beam splitter 416A be transmitted, and the second portion of collimated light beam is reflected.Reflecting part is directed on the first speculum 428A.Hop is directed onbeam combiner 424.

Thefirst speculum 428A is directed to folded light beam on the part of wavelength selector.

Thesecond gain equipment 412B produces the radiation by thesecond lens 414B collimation.The second collimated light beam is directed on thesecond beam splitter 416B, and the part of collimated light beam is transmitted again and second portion is reflected.Reflecting part is directed on the second speculum 428B.Hop is directed onbeam combiner 424.

Thesecond speculum 428B is directed to the second folded light beam onwavelength selector 418.

Wavelength selector 418 is got back to the corresponding first orsecond speculum 428A, 428B with the selected wavelength diffraction that incident beam antiparallel ground will be incident on each light beam on it, and its wavelength orientation that will select via the corresponding first orsecond beam splitter 416A, 416B is again got back to the corresponding first orsecond gain equipment 412A, 412B.

The first andsecond speculum 428A, 428B are controllable individually, make them to rotate around the axle perpendicular to radiation laser beam, in order to select to reflect back into the wavelength incorresponding gain equipment 412A, 412B.

The advantage of using independent scanning MEMS speculum and body grating is the cost that reduces and larger simplicity, and when using a plurality of resonator of a plurality of lasing light emitters, independent scanning MEMS speculum makes and realizes that existing parts are relative simple with body grating.A plurality of MEMS reflection mirror components can be used for using the grating (general the most expensive parts) of common body optics definition to adjust independent light beam.

Fig. 5 B illustrates the output spectrum of eachgain equipment 412A, 412B.The output spectrum of each gain equipment can be not identical; The output spectrum of each gain equipment has the wide bandwidth up to about 10nm.

Fig. 5 C illustrates the spectrum that is input in optical delivery fiber 422.Spectrum is included in two different peak values at different wavelength places, and each peak value has narrow bandwidth, and the peak wavelength of each peak value can be regulated by the rotation ofspeculum 428A, 428B.

Fig. 6 A illustrates tunable light source, and wherein lens 514 make from the radiation collimation of gain equipment 512 and collimated light beam is directed on fixation reflex type diffraction grating 518.The first rank diffracted beam is reflected back on diffraction grating 518 by speculum 528.By rotating mirror 528 capable of regulating wavelength.Because wavelength selectivity is stronger, this configuration can be showed the bandwidth less than previously described layout; The every round trip of the diffraction that wavelength is relevant occurs twice rather than once.Power output may be lower, because the zeroth order diffraction of the grating 518 of the light beam of next free speculum 528 reflections is not retained in resonator.Resonator is formed by the rear reflective surface 511 of reflecting surface, grating 518 and the gain equipment 512 of speculum 528.Grating 518 reflexes to the zeroth order radiation laser beam on lens 520.Lens 520 focus on the radiation that it is collected, and make it can be trapped in optical delivery fiber 522.Grating 518 serves as output coupler in this is arranged, removed the demand to beam splitter.

Fig. 6 B illustrates the output spectrum of the gain equipment 512 that comprises gain media.Can see, the output spectrum of the resonator that forms when the rear reflective surface 511 of the reflecting surface with by speculum 528, grating 518 and gain equipment 512 is relatively the time (as shown in Figure 6 C), and gain equipment has wide bandwidth.

Fig. 6 C is for four different angle θ in the orientation of wavelength selector 518₁, θ₂, θ₃, θ₄The spectrum of resonator is shown; The peak strength of spectrum appears at four different wavelength places.

Fig. 7 illustrates tunable light source, and wherein a pair ofgain equipment 612A, 612B produce the radiation that is collimated by the first andsecond lens 614A, 614B respectively.Each collimated light beam is directed to single wavelength selector 618.Preferably,wavelength selector 618 is reflection-type diffraction gratings.The first rank diffracted beam of each collimated light beam is directed oncorresponding speculum 628A, 628B; Eachspeculum 628A, 628B reflect back intowavelength selector 618 with the selected bandwidth of diffractedbeam.Wavelength selector 618 is got back to each folded light beam diffraction incorresponding gain equipment 612A, 612B viacorresponding lens 614A, 614B.Zero order diffraction beam from eachgain equipment 612A, 612B is directed inbeam combiner 624.

The output of each resonator is grouped together in beam combiner 624.Beam combiner 624 is optical polarization beam combiner preferably.

Then combination radiation frombeam combiner 124 passes isolator 626, and this prevents or reduce the feedback of radiation, and the image intensifer system of isolating pump light source and with pump light source, being coupled.

Condenser lens 620 redirects radiation, makes it can be trapped inoptical delivery fiber 622.

It is contemplated that aforementioned light source 10,110,210,310,410,510,610 pump light sources that can be used as image intensifer.Fig. 8 illustrates the schematic diagram of amplifier system.Shown image intensifer uses stimulated Raman scattering.Raman scattering is nonlinear effect, and thus, the high energy pumping radiation that is incident on medium is switched to different frequencies.Molecular vibration produce modification that the molecule excite decays to than low-lying level, and launch simultaneously photon.Frequency displacement is determined by the molecular vibration of material.If the signal photon is present in the optical fiber with pumping radiation, this emission can be stimulated; This is called as stimulated Raman scattering (SRS).Decay can cause to the frequency displacement of lower frequency (Stokes shift) or to the frequency displacement (anti-stokes frequency shifted) of higher frequency: usually, Stokes shift is used for providing the gain of light in the telecommunication application.Image intensifer system shown in Fig. 8 comprises optical fiber F, and input optical signal I/P is coupled in optical fiber F on direction.Pumping radiation can be coupled in optical fiber at output at input end or on " opposite pumping " inverse direction on " common pumping " direction.The amplified version of input optical signal (output optical signal O/P) is received at the output of optical fiber.

Operate at unimodal value wavelength place and have in approximately single pump light source 10,110,210,310,410,510,610 gains of light that can be provided on finite bandwidth of the bandwidth between 1-3nm.In order to realize the light amplification on wider bandwidth, can use two or more pump light sources, each light source has different peak wavelengths.Fig. 9 illustrates the use of four pump light sources, and shows the gain bandwidth of each pump light source to overall gain-bandwidth OG contribution.

In optional execution mode, light source 10,110,210,310,410,510,610 is used for the pumping erbium-doped fiber to produce " doped optical fibre amplifier ".Use wavelength selective coupler to mix with input signal from the radiation of light source.The light that mixes is directed in core in the sections of the optical fiber with bait ion.This radiation from light source is arrived the higher-energy state with the bait ion excitation.When the photon of the light signal at the wavelength place different from pump light during with the bait atomic interaction of being excited, the bait atom turns back to simultaneously than low-energy state, and the bait atomic emissions frequency/wavelength place and the phase place identical with the light signal that just is being exaggerated and the extra photon of direction.

It is contemplated that, the parts of light source will be arranged in the optical module shell, for example have such as the light through hole in the hole that be used for to receive optical fiber and be used for providing to the parts of light source " butterfly shape " packings of a plurality of electric through-holes of electric power and control.It is also contemplated that the thermoelectric (al) cooler of the temperature that is provided for control assembly.It is also contemplated that and can use the optional method that is used for coolant pump that is different from thermoelectric (al) cooler.

Can recognize, can carry out within the scope of the invention various changes, for example, pump light source can comprise a plurality of gain equipments, and each resonator of gain equipment can be arranged so that each gain equipment at different wavelength places or alternatively at identical substantially wavelength place " Emission Lasers ".

To recognize, as used herein, direction for example mention " top ", " bottom ", " front ", " back ", " end ", " side ", " inside ", " outside ", " top " and " bottom " with corresponding feature limits to such orientation, and only be used for these features are distinguished from each other out.In addition, will recognize, term " light " is not limited to visible spectrum, but is included in the electromagnetic radiation outside the visible spectrum of human eye, and particularly including infrared and ultra-violet radiation.

Claims (31)

Translated fromChinese

1.一种用在光放大器中的可调光源，包括：1. A tunable light source used in an optical amplifier, comprising:增益设备，其可操作来提供光放大，所述增益设备包括增益介质和第一反射表面；a gain device operable to provide optical amplification, the gain device comprising a gain medium and a first reflective surface;波长选择器，其选择来自所述增益设备的光的一部分；以及a wavelength selector that selects a portion of the light from the gain device; and输出耦合器，其将来自所述增益设备的光的一部分定向到所述波长选择器，并将另一部分定向到光传播器以用于耦合到光放大器，使得所述增益设备、输出耦合器和波长选择器形成谐振器。an output coupler that directs a portion of the light from the gain device to the wavelength selector and another portion to an optical spreader for coupling to an optical amplifier such that the gain device, output coupler, and The wavelength selector forms a resonator.2.如权利要求1所述的可调光源，其中所述输出耦合器包括分束器。2. The tunable light source of claim 1, wherein the output coupler comprises a beam splitter.3.如权利要求1或2所述的可调光源，包括两个或多个光谐振器，每个光谐振器包括形成相应的谐振器的部分的增益设备，其中从每个谐振器输出的光通过组合器耦合在一起并被定向到所述光传播器中。3. A tunable light source as claimed in claim 1 or 2, comprising two or more optical resonators, each optical resonator comprising a gain device forming part of the respective resonator, wherein the output from each resonator Light is coupled together by a combiner and directed into the light spreader.4.如权利要求1、2或3所述的可调光源，还包括用于改变来自所述增益设备的光的波长的致动器。4. A tunable light source as claimed in claim 1 , 2 or 3, further comprising an actuator for varying the wavelength of light from the gain device.5.如权利要求4所述的可调光源，其中所述致动器绕着垂直于光的传播方向的轴旋转所述波长选择器。5. The tunable light source of claim 4, wherein the actuator rotates the wavelength selector about an axis perpendicular to the direction of propagation of the light.6.如权利要求4所述的可调光源，其中所述致动器旋转光重定向器，该光重定向器优选地为反射镜，所述光重定向器将来自所述增益设备的光定向到所述波长选择器上，其中所述光重定向器绕着垂直于光的传播方向的轴旋转。6. The tunable light source of claim 4, wherein the actuator rotates a light redirector, preferably a mirror, that redirects light from the gain device directed onto the wavelength selector, wherein the light redirector is rotated about an axis perpendicular to the direction of propagation of the light.7.如权利要求4所述的可调光源，其中所述致动器在结构上使所述波长选择器变形以改变选定的波长。7. The tunable light source of claim 4, wherein the actuator structurally deforms the wavelength selector to change a selected wavelength.8.如权利要求7所述的可调光源，其中结构变形包括拉伸、压缩和/或弯曲所述波长选择器。8. The tunable light source of claim 7, wherein structural deformation includes stretching, compressing and/or bending the wavelength selector.9.如任一前述权利要求所述的可调光源，其中所述波长选择器包括反射型衍射光栅。9. A tunable light source as claimed in any preceding claim, wherein the wavelength selector comprises a reflective diffraction grating.10.一种用在光放大器中的可调光源，包括：10. A tunable light source used in an optical amplifier, comprising:两个或多个增益设备，其可操作来提供光放大，每个增益设备包括增益介质和第一反射表面；two or more gain devices operable to provide optical amplification, each gain device comprising a gain medium and a first reflective surface;两个或多个可致动波长选择器，每个可致动波长选择器选择来自所述增益设备之一的光的一部分；two or more actuatable wavelength selectors, each actuatable wavelength selector selects a portion of light from one of said gain devices;至少一个输出耦合器，其使得每个增益设备、输出耦合器和波长选择器形成谐振器，其中所述输出耦合器将来自每个增益设备的光的一部分定向到光传播器以用于耦合到光放大器。at least one output coupler such that each gain device, the output coupler and the wavelength selector form a resonator, wherein the output coupler directs a portion of the light from each gain device to the optical spreader for coupling to optical amplifier.11.如权利要求10所述的可调光源，其中所述至少一个输出耦合器包括至少一个衍射光栅。11. The tunable light source of claim 10, wherein the at least one output coupler comprises at least one diffraction grating.12.如权利要求10或11所述的可调光源，其中每个谐振器提供不同波长的光。12. A tunable light source as claimed in claim 10 or 11, wherein each resonator provides light of a different wavelength.13.如任一前述权利要求所述的可调光源，其中光重定向器将光定向到所述光传播器中。13. A dimmable light source as claimed in any preceding claim, wherein a light redirector directs light into the light spreader.14.一种用在光放大器中的可调光源，所述光源包括：14. An adjustable light source used in an optical amplifier, said light source comprising:增益设备，其可操作来提供光放大，所述增益设备包括增益介质以及第一端和第二端，所述第一端形成光谐振器的一端；a gain device operable to provide optical amplification, the gain device comprising a gain medium and a first end and a second end, the first end forming one end of an optical resonator;透镜，其用于准直从所述增益设备的第二端发射的辐射并将所述辐射定向到充当输出耦合器的分束器，用于允许辐射的一部分逸出所述光谐振器和用于将其余部分保留在所述光谐振器内；a lens for collimating radiation emitted from the second end of the gain device and directing the radiation to a beam splitter acting as an output coupler for allowing a portion of the radiation to escape the optical resonator and using while retaining the remainder within the optical resonator;反射型衍射光栅，其用于所述辐射的波长选择并形成所述光谐振器的第二端；以及a reflective diffraction grating for wavelength selection of said radiation and forming a second end of said optical resonator; and致动器，其耦合到所述反射型衍射光栅并可操作来改变所述波长选择。An actuator coupled to the reflective diffraction grating and operable to vary the wavelength selection.15.如权利要求14所述的用在光放大器中的可调光源，其中所述分束器将所述光谐振器中的辐射的保留部分反射到光重定向器上，例如反射镜上，所述光重定向器将所述辐射定向到所述反射型衍射光栅上，且其中所述致动器耦合到所述光重定向器。15. A tunable light source for use in an optical amplifier as claimed in claim 14, wherein said beam splitter reflects a reserved portion of the radiation in said optical resonator onto a light redirector, such as a mirror, The light redirector directs the radiation onto the reflective diffraction grating, and wherein the actuator is coupled to the light redirector.16.如权利要求14或15所述的可调光源，还包括：16. A dimmable light source as claimed in claim 14 or 15, further comprising:第二增益设备，其可操作来提供光放大，所述第二增益设备包括第二增益介质以及第一端和第二端，所述第一端形成第二光谐振器的一端；a second gain device operable to provide optical amplification, said second gain device comprising a second gain medium and a first end and a second end, said first end forming one end of a second optical resonator;第二透镜，其用于准直从所述第二增益设备的所述第二端发射的辐射并将所述辐射定向到充当第二输出耦合器的第二分束器上，用于允许辐射的一部分逸出所述第二光谐振器和用于将其余部分保留在所述第二光谐振器内；A second lens for collimating radiation emitted from said second end of said second gain device and directing said radiation onto a second beam splitter acting as a second output coupler for allowing radiation a portion of escaping the second optical resonator and for retaining the remaining portion within the second optical resonator;第二反射型衍射光栅，其用于所述辐射的波长选择并形成所述第二光谐振器的第二端；以及a second reflective diffraction grating for wavelength selection of said radiation and forming a second end of said second optical resonator; and第二致动器，其耦合到所述第二反射型衍射光栅并可操作来改变所述第二光谐振器的波长选择。A second actuator coupled to the second reflective diffraction grating and operable to vary the wavelength selection of the second optical resonator.17.如权利要求16所述的用在光放大器中的可调光源，其中第一分束器和第二分束器彼此偏移以防止将来自所述第一光谐振器或第二光谐振器中的一个的辐射耦合到所述第一光谐振器或第二光谐振器中的另一个中。17. The tunable light source for use in an optical amplifier as claimed in claim 16, wherein the first beam splitter and the second beam splitter are offset from each other to prevent resonating light from the first optical resonator or the second optical resonator The radiation from one of the resonators is coupled into the other of the first optical resonator or the second optical resonator.18.如权利要求16所述的用在光放大器中的可调光源，其中所述第一分束器和第二分束器在不同的方向上反射所述辐射的保留部分，可选地在相反的方向上反射所述辐射的保留部分。18. A tunable light source for use in an optical amplifier as claimed in claim 16, wherein said first and second beam splitters reflect the remaining portion of said radiation in different directions, optionally at The remaining portion of the radiation is reflected in the opposite direction.19.如权利要求16所述的用在光放大器中的可调光源，其中所述第一分束器和第二分束器在相同的方向反射所述辐射的保留部分。19. A tunable light source for use in an optical amplifier as claimed in claim 16, wherein said first and second beam splitters reflect a remaining portion of said radiation in the same direction.20.如权利要求16所述的用在光放大器中的可调光源，其中所述第一分束器将所述辐射的相应保留部分反射到第一光重定向器上，例如反射镜上，所述第一光重定向器将所述第一光谐振器中的辐射定向到所述第一反射型衍射光栅上，且其中所述第二分束器将所述辐射的相应保留部分反射到第二光重定向器上，例如反射镜上，所述第二光重定向器将所述第二光谐振器中的辐射定向到所述第二反射型衍射光栅上，且其中第一致动器和第二致动器分别耦合到所述第一光重定向器或第二光重定向器。20. A tunable light source for use in an optical amplifier as claimed in claim 16, wherein said first beam splitter reflects a respective reserved portion of said radiation onto a first light redirector, such as a mirror, The first light redirector directs radiation in the first optical resonator onto the first reflective diffraction grating, and wherein the second beam splitter reflects a corresponding remaining portion of the radiation onto On a second light redirector, such as a mirror, which directs radiation in the second optical resonator onto the second reflective diffraction grating, and wherein the first actuation A device and a second actuator are respectively coupled to the first light redirector or the second light redirector.21.如权利要求16所述的用在光放大器中的可调光源，其中所述第一分束器将所述辐射的相应保留部分反射到第一光重定向器上，例如反射镜上，所述第一光重定向器将所述第一光谐振器中的辐射定向到所述反射型衍射光栅上，且其中所述第二分束器将所述辐射的相应保留部分反射到第二光重定向器上，例如反射镜上，所述第二光重定向器将所述第二光谐振器中的辐射定向到所述反射型衍射光栅上，使得所述反射型衍射光栅形成所述第一光谐振器和第二光谐振器的部分，且其中所述第一致动器和第二致动器分别耦合到所述第一光重定向器或第二光重定向器。21. A tunable light source for use in an optical amplifier as claimed in claim 16, wherein said first beam splitter reflects a respective reserved portion of said radiation onto a first light redirector, such as a mirror, The first light redirector directs radiation in the first optical resonator onto the reflective diffraction grating, and wherein the second beam splitter reflects a corresponding remaining portion of the radiation to a second beam splitter. On a light redirector, such as a mirror, the second light redirector directs radiation in the second optical resonator onto the reflective diffraction grating such that the reflective diffraction grating forms the part of a first optical resonator and a second optical resonator, and wherein the first actuator and the second actuator are coupled to the first light redirector or the second light redirector, respectively.22.一种用在光放大器中的可调光源，所述可调光源包括：22. A tunable light source used in an optical amplifier, the tunable light source comprising:增益设备，其可操作来提供光放大，所述增益设备包括增益介质以及第一端和第二端，所述第一端形成光谐振器的一端；a gain device operable to provide optical amplification, the gain device comprising a gain medium and a first end and a second end, the first end forming one end of an optical resonator;透镜，其用于准直从所述增益设备的所述第二端发射的辐射并将所述辐射定向到用于所述辐射的波长选择并充当输出耦合器的反射型衍射光栅，允许所述辐射的一部分逸出所述光谐振器和用于将其余部分保留在所述光谐振器内；a lens for collimating radiation emitted from said second end of said gain device and directing said radiation to a reflective diffraction grating for wavelength selection of said radiation and acting as an output coupler, allowing said a portion of the radiation escapes the optical resonator and serves to retain the remainder within the optical resonator;光重定向器，例如反射镜，其形成所述光谐振器的第二端；a light redirector, such as a mirror, forming the second end of the optical resonator;致动器，其耦合到所述光重定向器并可操作来改变所述波长选择；an actuator coupled to the light redirector and operable to change the wavelength selection;第二增益设备，其可操作来提供光放大，所述第二增益设备包括第二增益介质以及第一端和第二端，所述第一端形成所述第二光谐振器的一端；a second gain device operable to provide optical amplification, the second gain device comprising a second gain medium and a first end and a second end, the first end forming one end of the second optical resonator;第二透镜，其用于准直从所述第二增益设备的第二端发射的辐射并将所述辐射定向到用于所述辐射的波长选择并充当第二输出耦合器的第二反射型衍射光栅，允许辐射的一部分逸出第二光谐振器和用于将其余部分保留在所述第二光谐振器内；A second lens for collimating and directing radiation emitted from the second end of the second gain device to a second reflective type for wavelength selection of the radiation and acting as a second output coupler a diffraction grating for allowing a portion of the radiation to escape the second optical resonator and for retaining the remainder within said second optical resonator;第二光重定向器，例如反射镜，其形成所述第二光谐振器的第二端；以及a second light redirector, such as a mirror, forming a second end of the second optical resonator; and第二致动器，其耦合到所述第二光重定向器并可操作来改变所述第二光谐振器的波长选择，其中所述反射型衍射光栅形成所述第一光谐振器和第二光谐振器的部分。a second actuator coupled to the second light redirector and operable to change the wavelength selection of the second optical resonator, wherein the reflective diffraction grating forms the first optical resonator and the second optical resonator part of the second optical resonator.23.如权利要求15到22中的任一项所述的可调光源，还包括用于组合来自所述第一光谐振器和第二光谐振器的辐射的组合器。23. A tunable light source as claimed in any one of claims 15 to 22, further comprising a combiner for combining radiation from the first and second optical resonators.24.如任一前述权利要求所述的可调光源，其中透镜将光定向到光纤中。24. A tunable light source as claimed in any preceding claim, wherein the lens directs the light into the fibre.25.如任一前述权利要求所述的可调光源，还包括用于当所述光源用在光放大器中时防止反馈的隔离器。25. A dimmable light source as claimed in any preceding claim, further comprising an isolator for preventing feedback when the light source is used in an optical amplifier.26.如权利要求4到25中的任一项所述的用在光放大器中的可调光源，其中所述致动器包括微机电系统MEMS。26. A tunable light source for use in an optical amplifier as claimed in any one of claims 4 to 25, wherein the actuator comprises a microelectromechanical system (MEMS).27.一种光放大器，其包括根据权利要求1到26中的任一项的可调光源。27. An optical amplifier comprising a tunable light source according to any one of claims 1 to 26.28.一种用于光信号的放大的拉曼放大器系统，其包括权利要求1到26中的任一项的可调光源作为泵浦光源。28. A Raman amplifier system for amplification of optical signals comprising the tunable light source of any one of claims 1 to 26 as a pump light source.29.一种如权利要求28所述的用于光信号的放大的拉曼放大器系统，其中两个或多个可调光源被组合以增加所述放大器系统的增益和光信号的放大。29. A Raman amplifier system for amplification of optical signals as claimed in claim 28, wherein two or more tunable light sources are combined to increase the gain of the amplifier system and the amplification of optical signals.30.一种如权利要求28所述的用于光信号的放大的拉曼放大器系统，其中两个或多个可调光源被组合以增加带宽，所述光信号可在所述带宽上放大。30. A Raman amplifier system for amplification of an optical signal as claimed in claim 28, wherein two or more tunable light sources are combined to increase the bandwidth over which said optical signal can be amplified.31.一种用于光信号的放大的掺饵光纤放大器系统，所述掺饵光纤放大器系统包括权利要求1到26中的任一项的可调光源作为泵浦光源以用于激发光纤中的饵原子。31. An erbium-doped fiber amplifier system for amplification of optical signals, said erbium-doped fiber amplifier system comprising the tunable light source according to any one of claims 1 to 26 as a pump light source for exciting the Bait atom.

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